Method of manufacturing low temperature sintered ceramic materials for use in solid dielectric capacitors or the like

ABSTRACT

A ceramic composition capable of sintering at a sufficiently low temperature to enable the use of a low cost base metal as the electrode material in the fabrication of capacitors. The major ingredient of the composition is expressed as Ba k-x  M x  O k  TiO 2 , where M is one or more of magnesium, zinc, strontium, and calcium, and where k, and x are numerals in the ranges of 1.00 to 1.04, and 0.02 to 0.05, respectively. To this major ingredient is added a minor proportion of a mixture of boron oxide and at least one of barium oxide, magnesium oxide, zinc oxide, strontium oxide, and calcium oxide. For the fabrication of coherently bonded bodies of this composition, as for use as the dielectric bodies of capacitors, the moldings of the mixture of the major ingredient and additive in finely divided form are sintered in a reductive or neutral atmosphere and then reheated at a lower temperature in an oxidative atmosphere. The sintering temperature can be so low (typically from 1050° to 1200° C.) that the moldings can be co-sintered with base metal electrodes buried therein without difficulties encountered heretofore.

This is a division of application Ser. No. 676,780, filed Nov. 30, 1984.

BACKGROUND OF THE INVENTION

Our invention relates to dielectric ceramic compositions that allow sintering or firing at lower temperatures than heretofore, and to a process for the fabrication of coherently bonded bodies of such compositions. The low temperature sintered ceramic materials of our invention find a typical application in solid dielectric capacitors, particularly in those of the monolithic or multilayered design, making possible the use of a base metal as the material for the film electrodes of such capacitors.

Multilayered ceramic capacitors are known which employ noble metals such as platinum and palladium as the electrode materials. For the manufacture of such multilayered capacitors, as heretofore practiced, there are first prepared green dielectric sheets from the proportioned ingredients for a dielectric ceramic material in finely divided form. An electroconductive paste containing powdered platinum or palladium is then "printed" on the green sheets in a desired pattern. Several such printed green sheets are stacked up, pressed together, and sintered in an temperature range of 1300° to 1600° C. in an oxidative atmosphere. This conventional method makes possible the simultaneous production (co-sintering) of the dielectric ceramic bodies and the film electrodes interleaved therein. It is also an acknowledged advantage of the known method that the noble metal electrodes are totally unaffected by the high temperature sintering in an oxidative atmosphere. Offsetting all these advantages is the expensiveness of the noble metals, which adds considerably to the costs of the multilayered ceramic capacitors.

A solution to this problem is found in Sakabe et al. U.S. Pat. No. 4,115,493 issued Sept. 19, 1978. This patent proposes a method of making a monolithic ceramic capacitor with use of a base metal such as nickel, iron or cobalt, or an alloy thereof, as the electrode material. According to this prior art method, a paste of a powdered base metal is screened on green dielectric sheets, and the pasted sheets are stacked, pressed together, and fired in a temperature range of 1300° to 1370° C. in a reductive atmosphere containing hydrogen. The oxidation of the pasted base metal particles is thus avoided.

We do, however, object to the Sakabe et al. method for the following reasons. We have discovered from experiment that the firing temperature range of 1300° to 1370° C. suggested by this prior art method leads to easy flocculation of the particles of nickel or like base metal pasted on the green dielectric sheets. The base metal particles have also been found to tend to diffuse into the ceramic bodies when fired in that temperature range. The flocculation and diffusion of the base metal particles are, of course, both undesirable as the resulting capacitors will not possess desired values of capacitance and insulation resistance.

SUMMARY OF THE INVENTION

Our invention provides a solution to the problem of how to reduce the sintering temperature of ceramic compositions, particularly in the manufacture of solid dielectric capacitors, to make possible the use of a low cost base metal as the electrode material without the noted difficulties encountered heretofore. The low temperature sintered ceramic material in accordance with our invention are also well calculated for the provision of capacitors of very favorable performance characteristics.

Stated in brief, a low temperature sintered ceramic material in accordance with our invention consists essentially of 100 parts by weight of a major ingredient expressed by the formula Ba_(k-x) M_(x) O_(k) TiO₂, where M is at least one of magnesium (Mg), zinc (Zn), strontium (Sr), and calcium (Ca), and where k and x are numerals in the ranges of 1.00 to 1.04, and 0.02 to 0.05, respectively, and 0.2 to 10.0 parts by weight of an additive mixture of 30 to 90 mole percent boron oxide (B₂ O₃) and 10 to 90 mole percent of at least one metal oxide (MO) selected from the group consisting of barium oxide (BaO), magnesium oxide (MgO), zinc oxide (ZnO), strontium oxide (SrO), and calcium oxide (CaO).

According to the method of our invention, for the fabrication of coherently bonded bodies of the above low temperature sintered ceramic material, there are first prepared the major ingredient, Ba_(k-x) M_(x) O_(k) TiO₂, and the additive mixture of B₂ O₃ and MO, in the above suggested proportions. After having been intimately mixed together, the major ingredient and additive are molded into bodies of desired shape and size. The moldings are subsequently sintered in a nonoxidative (i.e. neutral or reductive) atmosphere and then reheated in an oxidative atmosphere.

The dielectric ceramic composition of our invention, set forth in the foregoing, makes it possible to sinter the moldings in an nonoxidative atmosphere at temperatures less than 1200° C. A temperature range for this sintering operation is from 1050° C. to 1200° C. for the best results. The sintering temperatures of less than 1200° C. enable the use, in the fabrication of capacitors with the ceramic composition of our invention as the dielectric, of nickel or like low cost base metal as the electrode material without the difficulties that have been pointed out in connection with the prior art. The sintering temperature might be above 1200° C. Should it exceed 1300° C., however, the base metal particles pasted on dielectric bodies might flocculate or diffuse. Should the temperature be too low, on the other hand, then the dielectric bodies might not be sintered to maturity. Hence the preferred temperature range of 1050° to 1200° C. We recommend this temperature range not only because the base metal electrodes can be formed favorably but also because it realizes a substantial curtailment of the energy that has heretofore been consumed for firing the dielectric moldings.

The reheating of the sintered bodies in an oxidative atmosphere in accordance with the method of our invention is intended to compensate for the oxygen vacancies in the bodies that have been caused by the previous firing in a nonoxidative atmosphere and hence to increase their insulation resistance to a required degree. Thus the sintered bodies may be reheated at temperatures ranging from 500° C. to 1000° C. At any event, the reheating temperature should be lower than the preceding sintering temperature.

We also recommend that the periods of time for the sintering in a nonoxidative atmosphere and for the reheating in an oxidative atmosphere be minimums required for the accomplishment of the purposes for which the treatments are intended respectively. Experiment has proved that the moldings should be sintered at the maximum temperature for two to four hours, and subsequently reheated for 10 to 60 minutes, for the best results.

In addition to the advantages already set forth, our invention makes possible the provision of capacitors having specific dielectric constants of over 2000, dielectric losses of less than 2.5 percent, resistivity of over 1×10⁶ megohm-centimeters, and temperature dependences of capacitances of plus or minus 10 percent in a temperature range of -25° to +85° C.

The above and other features and advantages of our invention and the manner of realizing them will become more apparent, and the invention itself will best be understood, from a study of the following detailed description and appended claims, with reference had to the attached drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a sectional representation of an experimental multilayered ceramic capacitor employing the low temperature sintered ceramic material of our invention, the capacitor being representative of numerous test capacitors fabricated in the Example of the invention set forth subsequently; and

FIG. 2 is a graph plotting the average capacitance-temperature characteristic of test capacitors, each constructed as in FIG. 1, manufactured in Test No. 1 in the Example of our invention;

DETAILED DESCRIPTION

We have illustrated in FIG. 1 one of many similar multilayered ceramic capacitor fabricated in the subsequent Example of our invention by way of a possible application of our invention, each capacitor having its dielectric body formulated in accordance with the composition and method of our invention. Generally designated by the reference numeral 10, the representative capacitor is shown to have an alternating arrangement of three dielectric ceramic layers 12 and two film electrodes 14. The dielectric layers 12 have, of course, the low temperature sintered ceramic material of our invention. The film electrodes 14, which can be of a low cost base metal such as nickel, extend into the middle of the dielectric body 15, composed of the three dielectric layers 12, from the opposite sides thereof into a partly opposed relation with each other. A pair of conductive terminations 16 contact the respective-film electrodes 14. Each termination 16 comprises a baked on zinc layer 18, a plated on copper layer 20, and a plated on solder layer 22.

Typically, and as fabricated in the subsequent Examples of our invention, the intermediate one of the three dielectric layers 12 has a thickness of 0.02 millimeters. The area of that part of each film electrode 14 which is opposed to the other film electrode is 25 square millimeters (5×5 millimeters).

EXAMPLE

We fabricated 32 different sets of multilayered ceramic capacitors, each constructed as in FIG. 1, having their dielectric bodies 15 formulated in accordance with the compositions set forth in Table 1. The major ingredient of the ceramic compositions in accordance with our invention has been expressed as Ba_(k-x) M_(x) O_(k) TiO₂, where M is one or more of Mg, Zn, Sr, and Ca. Accordingly, in Table 1, we have given the specific atomic numbers, as represented by k-x,x, and k, of the elements Ba, M, and O of the major ingredient, as well as the total atomic numbers of Mg, Zn, Sr and Ca employed in various combinations as M. As regards the additive, the mixture of B₂ O₃ and MO, Table 1 specifies the proportion, in parts by weight, of this additive mixture with respect to 100 parts by weight of the major ingredient. Also given in Table 1 are the relative proportions, in mole percent, of B₂ O₃ and MO, and the relative proportions, in mole percent, of BaO, MgO, ZnO, SrO and CaO employed as MO.

                                      TABLE 1                                      __________________________________________________________________________     Ceramic Compositions                                                                                         Additive                                         Major Ingredient (100 wt. pt.)     Comp.                                       Test    -x                    Propn.                                                                              (mole %)                                                                             MO (mole %)                           No.                                                                                -k -  -x                                                                          Mg  Zn  Sr  Ca  Total                                                                               -k                                                                               (wt. pt.)                                                                           B.sub.2 O.sub.3                                                                   MO BaO                                                                               MgO                                                                               ZnO                                                                               SrO                                                                               CaO                       __________________________________________________________________________      1 1.02                                                                                0.005                                                                              0.005                                                                              0.005                                                                              0.005                                                                             0.02                                                                               1.04                                                                              1.0  30 70 50 30 20 -- --                         2 1.01                                                                                0.002                                                                              0.002                                                                              0.003                                                                              0.003                                                                             0.01                                                                               1.02                                                                              5.0  55 45 -- 10 10 40 40                         3 1.01                                                                               --  0.02                                                                               --  --  0.02                                                                               1.03                                                                              3.0  55 45 10 20 40 10 20                         4 1.01                                                                               --  0.02                                                                               0.01                                                                               --  0.03                                                                               1.04                                                                              3.0  25 75 40 -- 10 30 20                         5 1.00                                                                               0.02                                                                               --  --  --  0.02                                                                               1.02                                                                              1.0  35 65 60 -- 30 10 --                         6 1.00                                                                               0.02                                                                               --  --  --  0.02                                                                               1.02                                                                              1.0  35 65 -- 100                                                                               -- -- --                         7 1.00                                                                               --  --  0.01                                                                               0.02                                                                               0.03                                                                               1.03                                                                              0.2  55 45 30 30 40 -- --                         8 1.00                                                                               --  --  0.01                                                                               0.02                                                                               0.03                                                                               1.03                                                                              0.2  55 45 -- -- -- 40 60                         9 1.00                                                                               0.01                                                                               0.01                                                                               --  0.02                                                                               0.04                                                                               1.04                                                                              1.0  30 70 10 40 -- 30 20                        10 1.00                                                                               0.02                                                                               0.02                                                                               0.01                                                                               0.02                                                                               0.05                                                                               1.05                                                                              5.0  45 55 20 -- 70 -- 10                        11 0.99                                                                               --  --  --  0.02                                                                               0.02                                                                               1.01                                                                              10.0 55 45 80 10 -- 10 --                        12 0.99                                                                               --  --  --  0.02                                                                               0.02                                                                               1.01                                                                              10.0 55 45 -- -- -- -- 100                       13 0.99                                                                               0.02                                                                               0.01                                                                               --  --  0.03                                                                               1.02                                                                              1.0  90 10 70 -- -- 10 20                        14 0.99                                                                               0.02                                                                               0.01                                                                               --  --  0.03                                                                               1.02                                                                              1.0  90 10 -- 60 40 -- --                        15 0.99                                                                               0.01                                                                               --  0.01                                                                               0.01                                                                               0.03                                                                               1.02                                                                              0.0  -- -- -- -- -- -- --                        16 0.99                                                                               0.01                                                                               --  0.01                                                                               0.02                                                                               0.04                                                                               1.03                                                                              5.0  30 70 -- 70 10 -- 20                        17 0.99                                                                               0.02                                                                               --  --  0.02                                                                               0.04                                                                               1.03                                                                              12.0 55 45 10 10 80 -- --                        18 0.99                                                                               --  --  --  0.05                                                                               0.05                                                                               1.04                                                                              7.0  55 45 20 20 20 20 20                        19 0.98                                                                               --  --  0.02                                                                               --  0.02                                                                               1.00                                                                              0.2  90 10 -- 80 -- 20 --                        20 0.98                                                                               --  0.01                                                                               0.01                                                                               0.01                                                                               0.03                                                                               1.01                                                                              1.0  45 55 20 20 -- 60 --                        21 0.98                                                                               --  0.02                                                                               0.02                                                                               --  0.04                                                                               1.02                                                                              1.0  95  5 -- 10 10 -- 80                        22 0.97                                                                               0.01                                                                               0.01                                                                               0.01                                                                               --  0.03                                                                               1.00                                                                              10.0 30 70 -- 10 -- 80 10                        23 0.97                                                                               0.05                                                                               --  --  --  0.05                                                                               1.02                                                                              3.0  35 65 30 20 -- 20 30                        24 0.97                                                                               0.05                                                                               --  --  --  0.05                                                                               1.02                                                                              3.0  35 65 -- -- 100                                                                               -- --                        25 0.97                                                                               0.05                                                                               --  --  --  0.05                                                                               1.02                                                                              3.0  35 65 -- -- 50 -- 50                        26 0.97                                                                               0.01                                                                               0.01                                                                               0.01                                                                               0.02                                                                               0.05                                                                               1.02                                                                              3.0  85 15 -- -- 10 10 80                        27 0.97                                                                               0.02                                                                               0.02                                                                               0.01                                                                               0.01                                                                               0.06                                                                               1.03                                                                              0.2  55 45 20 20 20 20 20                        28 0.96                                                                               0.01                                                                               0.01                                                                               --  --  0.02                                                                               0.98                                                                              5.0  55 45 -- 10 30 50 10                        29 0.96                                                                               0.01                                                                               0.01                                                                               0.01                                                                               0.01                                                                               0.04                                                                               1.0                                                                               1.0  85 15 20 50 30 -- --                        30 0.96                                                                               --  --  0.05                                                                               --  0.05                                                                               1.01                                                                              1.0  45 55 30 10 10 20 30                        31 0.96                                                                               --  --  0.05                                                                               --  0.05                                                                               1.01                                                                              1.0  45 55 -- -- -- 100                                                                               --                        32 0.95                                                                               0.05                                                                               --  --  --  0.05                                                                               1.00                                                                              1.0  75 25 50 30 20 -- --                        __________________________________________________________________________

Thus, according to Test No. 1 of Table 1, for instance, the major ingredient was Ba₁.02 M₀.02 O₁.04 TiO₂ or, more specifically, Ba₁.02 Mg₀.005 Zn₀.005 Sr₀.005 Ca₀.005 O₁.04 TiO₂. One hundred parts by weight of this major ingredient was admixed with 1.0 part by weight of a mixture of 30 mole percent B₂ O₃ and 70 mole percent MO, the latter being, in this case, a mixture of 50 mole percent BaO, 30 mole percent MgO, and 20 mole percent ZnO.

For the fabrication of test capacitors of the Test No. 1 composition, we started with the preparation of the major ingredient, Ba₁.02 Mg₀.005 Zn₀.005 Sr₀.005 Ca₀.005 O₁.04 TiO₂. We first prepared 926.39 grams of BaCO₃, 0.94 gram of MgO, 1.88 grams of ZnO, 3.40 grams of SrCO₃, 2.32 grams of CaCO₃, and 368.44 grams of TiO₂, all with purities of over 99.0 percent. Expressed in mole parts, the relative proportions of the above prepared BaCO₃, MgO, ZnO, SrCO₃, CaCO₃, and TiO₂ were 1.02, 0.005, 0.005, 0.005, 0.005, and 1.0, respectively, aside from the impurities contained in the start materials. These start materials were wet mixed together for 15 hours. Then the mixture was dried at 150° C. for four hours, pulverized, and calcined in air at about 1200° C. for two hours. The major ingredient was thus obtained in finely divided form.

We prepared the additive of Test No. 1 by first preparing a mixture of 19.02 grams (30 mole percent) of B₂ O₃, 63.03 grams (35 mole percent) of BaCO₃, 7.76 grams (21 mole percent) of MgO, and 10.43 grams (14 mole percent) of ZnO. To this mixture we added 300 cubic centmeters of alcohol, and the resulting mixture was agitated for 10 hours in a polyethylene pot with alumina balls. Then the mixture was air fired at 1000° C. for two hours. Then, charged into an alumina pot together with 300 cubic centimeters of water, the mixture was crushed with alumina balls for 15 hours. Then the crushed mixture was dried at 150° C. for four hours. There was thus obtained the desired additive mixture of 30 mole percent B₂ O₃ and 70 mole percent MO (35 mole percent BaO, 21 mole percent MgO, and 14 mole percent ZnO) in finely divided form.

Then 1000 grams of the above prepared major ingredient and 10 grams (one weight percent) of the above prepared additive was mixed together. Further, to this mixture, we added 15 percent by weight of an organic binder and 50 percent by weight of water with respect to the total amount of the major ingredient and the additive. The organic binder was an aqueous solution of acrylic ester polymer, glycerine, and condensed phosphate. All these were ball milled into a slurry. Then this slurry was defoamed in vacuum. Then the deformed slurry was introduced into a reverse roll coater thereby to be shaped into a thin, continuous strip on an elongate strip of polyester film. Then the continuous strip of the slurry was dried at 100° C. on the polyester film. The green (unsintered) ceramic strip thus obtained, about 25 microns thick, was subsequently cut into "squares" sized 10 by 10 centimeters.

For the fabrication of the base metal film electrodes 14, we prepared 10 grams of nickel in finely divided form, with an average particle size of 1.5 microns, and a solution of 0.9 gram of ethyl cellulose in 9.1 grams of butyl "Carbitol" (trademark for diethylene glycol monobutyl ether). Both were agitated for 10 hours into an electroconductive paste. This paste was "printed" on one surface of each green ceramic sheet, which had been prepared as above, through a screen having approximately 50 rectangular perforations each sized 7 by 14 millimeters. Then, after drying the printed paste, two green ceramic sheets were stacked, with their printings directed upwardly, and with the printings on the two sheets offset from each other to an extent approximately one half of their longitudinal dimension. Further, four green ceramic sheets each with a thickness of 60 microns were stacked on each of the top and bottom surfaces of the two printed ceramic sheets. Then the stacked sheets were pressed in their thickness direction under a pressure of approximately 40 tons at 50° C., thereby bonding the stacked sheets together. Then the bonded sheets were cut in a latticed pattern into approximately 100 pieces.

We employed a furnace capable of atmosphere control for co-firing the above prepared green dielectric bodies and what were to become film electrodes buried therein. The bodies were first air heated to 600° C. at a rate of 100° C. per hour, thereby driving off the organic binder that had been used for providing the slurry of th powdered major ingredient and additive. Then, with the furnace atmosphere changed from air to a reductive (nonoxidative) atmosphere consisting of two percent by volume of molecular hydrogen and 98 percent by volume of molecular nitrogen, the furnace temperature was raised from 600° C. to 1160° C. at a rate of 100° C. per hour. The maximum temperature of 1160° C., at which the ceramic bodies could be sintered to maturity, was maintained for three hours. Then the furnace temperature was lowered to 600° C. at a rate of 100° C. per hour. Then the furnace atmosphere was again changed to air (oxidative atmosphere), and the temperature of 600° C. was maintained for 30 minutes in that atmosphere for the oxidative heat treatment of the sintered bodies. Then the furnace temperature was allowed to lower to room temperature. There were thus obtained the dielectric ceramic bodies 15, FIG. 1, co-sintered with the film electrodes 14 buried therein.

We proceeded to the production of the pair of conductive terminations 16 on both sides of each ceramic body 15. First, for the fabrication of the inmost zinc layers 18, an electroconductive paste composed of zinc, glass frit, and vehicle was coated on both sides of each ceramic body 15. The coatings were dried and air heated at 550° C. for 15 minutes, thereby completing the zinc layers 18, each in direct contact with one of the two film electrodes 14 buried in each ceramic body 15. Then the intermediate copper layers 20 were formed on the zinc layers 18 by electroless plating. The outermost solder layers 22 were formed subsequently by electroplating a lead-tin alloy onto the copper layers 20.

There were thus completed the fabrication of multilayered ceramic capacitors, each constructed as in FIG. 1, of Test No. 1. The composition of the sintered ceramic bodies 10 is substantially the same as that before sintering. Essentially, therefore, it is reasoned that the ceramic bodies 15 are of perovskite structures, with the additive (mixture of 30 mole percent B₂ O₃, 35 mole percent BaO, 21 mole percent MgO and 14 mole percent ZnO) substantially uniformly dispersed among the crystal grains of the major ingredient (Ba₁.02 Mg₀.005 Zn₀.005 Sr₀.005 Ca₀.005 O₁.04 TiO₂).

We have so far described the method of fabricating multilayered ceramic capacitors in accordance with the composition of Test No. 1. As regards the other ceramic compositions of Table I, designated Tests Nos. 2 through 32, we manufactured similar multilayered ceramic capacitors through exactly the same procedure as that of Test No. 1 except for changes in the temperature of firing (sintering) in the reductive (nonoxidative) atmosphere.

The multilayered ceramic capacitors of Tests Nos. 1 through 32 were then tested as to their specific dielectric constants, dielectric losses, resistivities, and percent changes in capacitances from thoese at +20° C. to those at -25° C. and +85° C. We measured these electrical properties of the test capacitors by the following methods:

1. Specific Dielectric Constant

The capacitance of each test capacitor was first measured at a temperature of 20° C., a frequency of one kilohertz, and an effective voltage of 0.5 volt. Then the specific dielectric constant was computed from the measured value of capacitance, and the area (25 square millimeters) of each of the opposed parts of the film electrodes 14, and the thickness (0.02 millimeter) of that ceramic layer 12 which intervenes between the film electrodes.

2. Dielectric Loss

Under the same conditions as the specific dielectric constant.

3. Resistivity

Resistance between the pair of terminations 16 of each test capacitor was measured after the application of a direct current at 50 volts for one minute. Then resistivity was computed from the measured resistance value and size of each test capacitor.

4. Capacitance-Temperature Characteristic

The test capacitors were introduced into a thermostatic oven, and at temperatures of -25°, 0°, +20°, +40°, +60°, and +85° C., their capacitances were measured at a frequency of one kilohertz and an effective voltage of 0.5 volt. Then the percent changes of the capacitances from those at 20° C. to the other specified temperatures were ascertained.

Table 2 gives the results of the measurements by the above methods. It will be seen from this table that the specific dielectric constants of the Test No. 1 capacitors, for instance, averaged 3070, their dielectric losses 1.2 percent, their resistivities 2.5×10⁶ megohm-centimeters, and their percent variations of capacitances from those at +20° C. to those at -25° and +85° C., -8.8 and +4.8 percent, respectively.

FIG. 2 graphically represents the average percent variations of the capacitances of the Test No. 1 capacitors at the above specified temperatures from their capacitances at +20° C. It will be noted that the capacitance variations in the temperature range of -25° to -85° C. are all in the range of plus and minus 10 percent. This capacitance-temperature characteristic was typical of all the capacitors of Tests Nos. 1 through 32; that is, if the percent variations of the capacitances of any groups of test capacitors at -25° and +85° C. were within plus and minus 10 percent, so were their capacitance variations at the other temperatures in between.

                                      TABLE 2                                      __________________________________________________________________________     Firing Temperatures & Capacitor Characteristics                                       Capacitor Characteristics                                                  Firing                                                                             Specific                                                                             Dielectric                                                        Test                                                                              Temp.                                                                              Dielectric                                                                           Loss  Resistivity                                                                           Capacitance Variations (%)                           No.                                                                               (°C.)                                                                       Constant                                                                             (%)   (megohm-cm)                                                                           At -25° C.                                                                     At +85° C.                             __________________________________________________________________________      1 1160                                                                               3070  1.2   2.5 × 10.sup.6                                                                  -8.8   +4.8                                           2 1100                                                                               2900  1.0   6.3 × 10.sup.6                                                                  -11.8  +8.7                                           3 1120                                                                               2960  0.8   6.2 × 10.sup.6                                                                  -9.2   +3.5                                           4 1250                                                                               Not coherently bonded on firing.                                         5 1160                                                                               3000  1.0   4.3 × 10.sup.6                                                                  -9.5   -0.8                                           6 1160                                                                               2980  1.2   4.1 × 10.sup.6                                                                  -9.4   -1.7                                           7 1180                                                                               3280  1.3   2.6 × 10.sup.6                                                                  -6.1   +3.5                                           8 1180                                                                               3290  1.3   2.7 × 10.sup.6                                                                  -6.2   +3.8                                           9 1160                                                                               3020  1.2   4.8 × 10.sup.6                                                                  -6.8   -4.4                                          10  1250                                                                              Not coherently bonded on firing.                                        11 1070                                                                               2890  1.9   2.5 × 10.sup.6                                                                  -6.2   +2.5                                          12 1070                                                                               2900  1.7   2.7 × 10.sup.6                                                                  -6.7   +3.1                                          13 1150                                                                               3040  1.6   4.3 × 10.sup.6                                                                  -8.2   -4.5                                          14 1150                                                                               3010  1.5   4.0 × 10.sup.6                                                                  -8.7   -4.8                                          15 1250                                                                               Not coherently bonded on firing.                                        16 1090                                                                               2930  1.4   6.2 × 10.sup.6                                                                  -8.3   -2.6                                          17 1070                                                                               2690  2.8   7.5 × 10.sup.5                                                                  -9.3   -6.3                                          18 1070                                                                               2830  1.3   4.2 × 10.sup.6                                                                  -9.0   -4.7                                          19 1170                                                                               3210  1.7   2.3 × 10.sup.6                                                                  -7.3   +9.5                                          20 1070                                                                               3120  1.1   4.2 × 10.sup.6                                                                  -7.5   +1.6                                          21 1140                                                                               2980  2.9   4.1 × 10.sup.6                                                                  -6.8   -2.3                                          22 1070                                                                               2840  2.2   2.0 × 10.sup.6                                                                  -9.2   -6.4                                          23 1130                                                                               2660  0.8   6.5 × 10.sup.6                                                                  -9.4   -9.1                                          24 1130                                                                               2630  0.9   6.2 × 10.sup.6                                                                  -9.2   -9.4                                          25 1130                                                                               2650  0.9   6.4 × 10.sup.6                                                                  -9.3   -8.9                                          26 1110                                                                               2790  1.2   6.2 × 10.sup.6                                                                  -9.4   -4.7                                          27 1180                                                                               2820  1.4   2.1 × 10.sup.6                                                                  -13.8  -7.4                                          28 1100                                                                               2920  8.3   3.8 × 10.sup.6                                                                  -8.4   +1.5                                          29 1140                                                                               3000  1.4   4.0 × 10.sup.3                                                                  -7.2   -3.4                                          30 1150                                                                               2900  1.1   4.2 × 10.sup.6                                                                  -9.3   +1.2                                          31 1150                                                                               2920  1.0   4.3 × 10.sup.6                                                                  -9.4   +3.2                                          32 1140                                                                               2750  1.0   4.4 × 10.sup.6                                                                  -9.2   -9.5                                          __________________________________________________________________________

Before proceeding further with the examination of Table 2, we will determine the acceptance criteria of the four electrical properties in question of capacitors in general as follows:

Specific dielectric constant, at least 2000.

Dielectric loss, not more than 2.5 percent.

Resistivity, at least 1×10⁶ megohm-centimeters.

Temperature dependence of capacitance, within plus and minus 10 percent.

A reconsideration of Table 2 in light of the above established criteria of favorable capacitor characteristics will reveal that the capacitors of Tests Nos. 2, 4, 10, 15, 17, 21, 27 and 28 do not meet these criteria. Accordingly, the corresponding ceramic compositions of Table 1 fall outside the scope of our invention.

Now, let us study the ceramic compositions of Table 1 and the corresponding capacitor characteristics of Table 2 in more detail. The ceramic composition of Test No. 15 contained no additive specified by our invention. The dielectric bodies formulated accordingly were not coherently bonded on firing at a temperature as high as 1250° C. Consider the ceramic composition of Test No. 7 for comparison. It contained 0.2 part by weight of the additive with respect to 100 parts by weight of the major ingredient. Even though the firing temperature was as low as 1180° C., the Test No. 7 composition could be processed into capacitors having the desired electrical characteristics. We set, therefore, the lower limit of the possible proportions of the additive at 0.2 part by weight with respect to 100 parts by weight of the major ingredient.

The Test No. 17 ceramic composition contained as much as 12 parts by weight of the additive with respect to 100 parts by weight of the major ingredient. The resulting capacitors have an average dielectric loss of 2.8 percent, which is higher than the above established criterior. However, when the proportion of the additive was reduced to 10 parts by weight, as in the Test No. 11 ceramic composition, then the resulting capacitors have the desired dielectric loss and other characteristics. Accordingly, the upper limit of the possible proportions of the additive is set at 10 parts by weight with respect to 100 parts by weight of the major ingredient.

As for the major ingredient, Ba_(k-x) M_(x) O_(k) TiO₂, the value of x was set at 0.01 in Test No. 2. In the resulting capacitors, the average variation of capacitances at -25° C. is -11.8 percent, outside the desired range of plus and minus 10 percent. However, when the value of x was increased to 0.02, as in Test No. 1, then the desired criteria of capacitance-temperature characteristics and other properties could all be achieved. Thus the lowermost possible value of x is 0.02. The Test No. 27 composition had the value of x set at as high as 0.06. In the resulting capacitors, the average variation of capacitance at -25° C. is -13.8 percent, which also is outside the desired range of plus and minus 10 percent. In Tests Nos. 18, and 23 to 26, the value of x was set slightly lower, at 0.05, and the resulting capacitors possess all the desired electrical characteristics. The uppermost possible value of x is therefore 0.05.

Mg, Zn, Sr, and Ca, represented by the capital M in the formula of the major ingredient, all belong to Group II of the Periodic Table, and their functions in the ceramic compositions of our invention are analogous. Consequently, any one or more of these metals may be employed in each composition. The results of Table 2 prove that the value of x can be in the range of 0.02 to 0.05 regardless of the number of the listed metals employed.

The value of k in the formula of the major ingredient was set at 0.98 in Test No. 28, with the result that the average resistivity of the associated capacitors is 3.8×10³ megohm-centimeters, much lower than the required minimum, and the average dielectric loss of the associated capacitors is 8.3 percent, much higher than the required maximum. However, the desired criteria of resistivity, dielectric loss, and other properties were all achieved when k was set at 1.00 as in Test No. 19. The lowermost possible value of k is therefore 1.00. On the other hand, when the value of k was increased to 1.05, as in Test No. 10, the resulting dielectric bodies were not coherently bonded on firing. As in Test No. 1, however, capacitors of the desired electrical characteristics could be produced when the value of k was set at 1.04. Accordingly, the uppermost possible value of k is 1.04.

Concerning the composition of the additive, the mixture of B₂ O₃ and MO (one or more of BaO, MgO, ZnO, SrO and CaO), it will be noted from Test No. 4 that when the proportion of B₂ O₃ with respect to that of MO was set at 25 mole percent, the dielectric bodies of the resulting composition were not coherently bonded on firing at a temperature as high as 1250° C. However, when the proportion of B₂ O₃ was increased at 30 mole percent, as in Test No. 1, the corresponding dielectric bodies could be sintered to maturity at a reduced temperature of 1160° C., to provide capacitors having the desired electrical characteristics. On the other hand, when the B₂ O₃ proportion was set at as high as 95 mole percent as in Test No. 21, the average dielectric loss of the resulting capacitors was as poor as 2.9 percent. The desired electrical characteristics were all obtained when the B₂ O₃ proportion was up to only 90 mole percent as in Test No. 13. We conclude from these findings that the acceptable range of the proportions of B₂ O₃ is from 30 to 90 mole percent and, consequently, that the acceptable range of the proportions of MO is from 10 to 70 mole precent.

As MO, there may be employed only one of BaO, MgO, SrO, ZnO and CaO, as in Tests Nos. 6, 12, 24 and 31, or two or more of these metal oxides as in the other Tests, for the provision of capacitors of the desired characteristics in accordance with our invention.

Although we have disclosed our invention in terms of specific Example thereof, we understand that our invention is not to be limited by the exact details of such disclosure but is susceptible to a variety of modifications within the usual knowledge of the ceramics or chemicals specialist without departing from the scope of the invention.

The following, then, is a brief list of such possible modifications:

1. The low temperature sintered ceramic material of our invention might include various additives not disclosed herein. An example is a mineralizer such as manganese dioxide. Used in a proportion (preferably from 0.05 to 0.10 percent by weight) not adversely affecting the desired properties of the inventive ceramic compositions, such a mineralizer would improve their sinterability.

2. The start materials for the major ingredient of the ceramic compositions of our invention might be substances other than those employed in the Example herein, examples being oxides such as BaO, SrO and CaO, hydroxides, etc. The start materials for the additive of the ceramic compositions of our invention might also be compounds such as oxides and hydroxides other than those disclosed herein.

3. The temperature of reheating in an oxidative atmosphere might be determined variously in consideration of such factors as the particular base metal electrode material in use and the degree of oxidation required for the ceramic materials.

4. The temperature of co-sintering in a nonoxidative atmosphere might also be changed in consideration of the particular electrode material in use.

5. The low temperature sintered ceramic material of our invention might be used as the dielectric bodies of capacitors other than those of the multilayered type disclosed herein.

6. The atmosphere of sintering could be neutral. 

What we claim is:
 1. A process for the fabrication of coherently bonded bodies of a low temperature sintered ceramic material, for particular use as the dielectric bodies of capacitors, which comprises:forming green bodies of desired shape and size from a mixture of 100 parts by weight of Ba_(k-x) M_(x) O_(k) TiO₂ in finely divided form, where M is at least either of magnesium, zinc, strontium and calcium, where k is a numeral in the range of 1.00 to 1.04 and where x is a numeral in the range of 0.02 to 0.05, and 0.2 to 10.0 parts by weight of an additive in finely divided form composed of 30 to 90 mole percent boron oxide and 10 to 70 mole percent of at least one metal oxide selected from the group consisting of barium oxide, magnesium oxide, zinc oxide, strontium oxide, and calcium oxide for providing upon firing coherently bonded dielectric bodies with a specific dielectric constant in excess of 2000, dielectric losses of less than 2.5 percent, resistivity of over 1×10⁶ megohm-centimeters and capacitance temperature dependence of + or -10% in a temperature range of -25° to +85° C.; sintering the green bodies to maturity in a nonoxidative atmosphere at a temperature not to exceed 1300° C.; and re-heating the sintered bodies in an oxidative atmosphere at a temperature lower than the preceding sintering temperature.
 2. A process for the fabrication of coherently bonded bodies of a low temperature sintered ceramic material as set forth in claim 1, wherein the bodies are sintered in a temperature range of 1050° to 1200° C.
 3. A process for the fabrication of coherently bonded bodies of a low temperature sintered ceramic material as set forth in claim 2, wherein the sintered bodies are reheated in a temperature range of 500° to 1000° C. 